Original file (1,543 × 1,002 pixels, file size: 70 KB, MIME type: image/jpeg)
Click on a date/time to view the file as it appeared at that time.
Date/Time | Thumbnail | Dimensions | User | Comment | |
---|---|---|---|---|---|
current | 17:49, 24 September 2020 |
![]() | 1,543 × 1,002 (70 KB) | Interferometrist | {{subst:Upload marker added by en.wp UW}} {{Information |Description = {{en|Factor by which a half-wave dipole must be shorter than lambda/2 in order to obtain resistive feedpoint impedance (cancellation of reactance). Computed using the induced EMF method as described in Dipole antenna#Induced EMF method. At larger diameters, the approximations used by this method break down, where the graph becomes dashed.}} |Source = Plotted on basis of equations s... |
The following other wikis use this file:
Original file (1,543 × 1,002 pixels, file size: 70 KB, MIME type: image/jpeg)
Click on a date/time to view the file as it appeared at that time.
Date/Time | Thumbnail | Dimensions | User | Comment | |
---|---|---|---|---|---|
current | 17:49, 24 September 2020 |
![]() | 1,543 × 1,002 (70 KB) | Interferometrist | {{subst:Upload marker added by en.wp UW}} {{Information |Description = {{en|Factor by which a half-wave dipole must be shorter than lambda/2 in order to obtain resistive feedpoint impedance (cancellation of reactance). Computed using the induced EMF method as described in Dipole antenna#Induced EMF method. At larger diameters, the approximations used by this method break down, where the graph becomes dashed.}} |Source = Plotted on basis of equations s... |
The following other wikis use this file: